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(2)

Application Note AN4138

Design Considerations for Battery Charger Using Green Mode Fairchild Power Switch (FPS TM )

Abstract

This application note presents practical design consider- ations for battery chargers employing Green Mode FPS (Fairchild Power Switch). It includes designing the transformer and output filter, selecting the components and implementing constant current / constant voltage control.

The step-by-step design procedure described in this paper will help engineers design battery chargers more easily. In order to make the design process more efficient, a software design tool, FPS design assistant that contains all the equations described in this paper is also provided. The design procedure is verified through an experimental prototype converter.

Rev. 1.0.0

1. Introduction

As penetration rates of portable electronics devices such as cellular phones, digital cameras or PDAs have increased significantly, the demands for low cost battery chargers are rising these days. Fairchild Power Switch (FPS) reduces total component count, design size, weight and, at the same time increases efficiency, productivity, and system reliability when compared to a discrete MOSFET and controller or RCC switching converter solution. Table 1 shows the FPS lineup for a battery charger application. Figure 1 shows the schematic of the basic battery charger using FPS, which also serves as the reference circuit for the design process

described in this paper. An experimental flyback converter from the design example has been built and tested to show the validity of the design procedure.

Table 1. FPS lineup for a battery charger Figure 1. Basic Battery charger Using FPS

Np NS

Rsn Csn - Vsn

+ VDC

+ -

AC line

Dsn

DR

CO

Drain

Vcc GND FB

FPS

Na Da Ra

Ca

H11A817A Rd Bridge

rectifier

diode VO

LP

CP

CB CDC

IO

IOref

VOref

Current Controller

Voltage Controller

Vbias

H11A817A

Device Switching frequency

Current limit

Rdson (typ.) FSDH0165 100 kHz 0.35 A 15.6 Ω

FSD311 67 kHz 0.55 A 14 Ω

FSD200 134 kHz 0.32 A 28 Ω

FSD210 134 kHz 0.32 A 28 Ω

(3)

2. Step-by-step Design Procedure

Figure 2. Flow chart of design procedure

In this section, a design procedure is presented using the schematic of Figure 1 as a reference. Figure 2 illustrates the design flow chart. The detailed design procedures are as follows:

(1) STEP-1 : Define the system specifications - Line voltage range (Vlinemin and Vlinemax).

- Line frequency (fL).

- Maximum output power (Po).

- Estimated efficiency (Eff) : It is required to estimate the power conversion efficiency to calculate the maximum input power. In the case of a battery charger, the efficiency is relatively low due to the low output voltage and loss in the output current sense resistor. The typical efficiency is about 0.65-0.7.

With the estimated efficiency, the maximum input power is given by

(2) STEP-2 : Determine DC link capacitor (CDC) and the DC link voltage range.

It is typical to select the DC link capacitor as 2-3uF per watt of input power for universal input range (85-265Vrms) and 1uF per watt of input power for European input range (195V- 265Vrms). With the DC link capacitor chosen, the minimum link voltage is obtained as

where Dch is the DC link capacitor charging duty ratio defined as shown in Figure 3, which is typically about 0.2 and Pin, Vlinemin and fL are specified in step-1.

The maximum DC link voltage is given as

where Vlinemax is specified in step-1.

Figure 3. DC Link Voltage Waveform 1. Determine the system specifications

(Vlinemin, Vlinemax, fL, Po, Eff)

2. Determine DC link capacitor (CDC) and DC link voltage range

3. Determine the reflected output voltage (VRO)

6. Determine the proper core and the minimum primary turns (Npmin)

7. Determine the number of turns for each output

8. Determine the wire diameter for each winding

9. Choose the proper rectifier diode for each output

10. Determine the output capacitor

11. Design the RCD snubber

12. Control Circuit design 5. Choose proper FPS considering input

power and Idspeak

4. Determine the transformer primary side inductance (Lm) and maximum duty (Dmax)

Is the winding window area (Aw) enough ?

Design finished

Y

N

Is it possible to change the core ? Y

N

Pin Po

Eff ---

= (1)

VDCmin 2⋅(Vlinemin)2 Pin(1Dch) CDCfL ---

= (2)

VDCmax= 2Vlinemax (3)

DC link voltage Minimum DC link voltage

T1 T2 Dch = T1 / T2

= 0.2

(4)

(3) STEP-3 : Determine the reflected output voltage (VRO).

When the MOSFET in the FPS is turned off, the input voltage (VDC) together with the output voltage reflected to the primary (VRO) are imposed on the MOSFET as shown in Figure 4. After determining VRO, the maximum nominal MOSFET voltage (Vdsnom) is obtained as

where VDCmax is specified in equation (3). The typical value for VRO is 65-85V.

Figure 4. The output voltage reflected to the primary

(4) STEP-4 : Determine the transformer primary side inductance (Lm) and the maximum duty ratio (Dmax).

A Flyback converter has two kinds of operation modes;

continuous conduction mode (CCM) and discontinuous conduction mode (DCM). The operation changes between CCM and DCM as the load condition and input voltage vary and each operation mode has their own advantages and disadvantages, respectively. The transformer size can be reduced using DCM because the average energy stored is lower compared to CCM. However, DCM inherently causes higher RMS current, which increases the conduction loss of the MOSFET and the current stress on the output capacitors.

For low power applications under 10W where the MOSFET conduction loss is not so severe, it is typical to design the converter to operate in DCM for the entire operating range, or to operate in CCM only for low input voltage conditions in order to minimize the transformer size.

Figure 5. Simplified flyback converter

The design procedures for CCM and DCM are slightly different. Once the reflected output voltage (VRO) is determined in step-3, the flyback converter can be simplified as shown in Figure 5 by neglecting the voltage drops in MOSFET and diode.

For CCM operation, the maximum duty ratio is given by

where VDCmin and VRO are specified in equations (2) and step-3, respectively.

For DCM operation, the maximum duty ratio should be determined as smaller than the value obtained in equation (5). By reducing Dmax, the transformer size can be reduced.

However, this increases the RMS value of the MOSFET drain current and Dmax should be determined by trade-off between the transformer size and MOSFET conduction loss.

With the maximum duty ratio, the primary side inductance (Lm) of the transformer is obtained. The worst case in designing Lm is full load and minimum input voltage Vdsnom = VDCmax+VRO (4)

- VR O

+ VD C

+ -

D ra in

G N D F P S

+ Vd s

-

0 V VD C VR O

Lm VDCmin

VRO

Ids

ID Im

Im

Im

Ids

Ids Dmax

Dmax

ID

ID

min DC RO

RO

V V

V

= +

min DC RO

RO

V V

V

≤ +

Dmax VRO

VRO+VDCmin ---

= (5)

(5)

condition. Therefore, Lm is obtained in this condition as

where VDCmin is specified in equation (2), Dmax is specified in equation (5), Pin is specified in step-1, fs is the switching frequency of the FPS device and KRF is the ripple factor in full load and minimum input voltage condition, defined as shown in Figure 6. For DCM operation, KRF = 1 and for CCM operation KRF < 1. The ripple factor is closely related to the transformer size and the RMS value of the MOSFET current. In the case of low power applications such as battery chargers, a relatively large ripple factor is used in order to minimize the transformer size. It is typical to set KRF = 0.5- 0.7 for the universal input range and KRF = 1.0 for the European input range.

Once Lm is determined, the maximum peak current and RMS current of the MOSFET in normal operation are obtained as

where Pin, VDCmin, Dmax and Lm are specified in equations (1), (2), (5) and (6) respectively and fs is the FPS switching frequency.

Figure 6. MOSFET Drain Current and Ripple Factor (KRF)

(5) STEP-5 : Choose the proper FPS considering input power and peak drain current.

With the resulting maximum peak drain current of the MOSFET (Idspeak) from equation (7), choose the proper FPS of which the pulse-by-pulse current limit level (Iover) is higher than Idspeak. Since FPS has ± 12% tolerance of Iover, there should be some margin in choosing the proper FPS device.

(6) STEP-6 : Determine the proper core and the minimum primary turns.

Table 2 shows the commonly used cores for battery chargers with output power under 10W. The cores recommended in table 2 are typical for the universal input range and 100kHz switching frequency.

With the chosen core, the minimum number of turns for the transformer primary side to avoid the core saturation is given by

where Lm is specified in equation (6), Iover is the FPS pulse- by-pulse current limit level, Ae is the cross-sectional area of the core as shown in Figure 7 and Bsat is the saturation flux density in tesla. Figure 8 shows the typical characteristics of ferrite core from TDK (PC40). Since the saturation flux density (Bsat) decreases as the temperature goes high, the high temperature characteristics should be considered.

If there is no reference data, use Bsat =0.3~0.35 T. Since the MOSFET drain current exceeds Idspeak and reaches Iover in a transition or fault condition, Iover is used in equation (11) instead of Idspeak to prevent core saturation during transition.

Figure 7. Window Area and Cross Sectional Area Lm (VDCminDmax)2

2PinfsKRF ---

= (6)

Idspeak IEDCI

---2 +

= (7)

Idsrms 3 I( EDC)2I

---2

  2

+ Dmax

---3

= ( )8

IEDC Pin

VDCminDmax ---

= (9)

I VDC

min Dmax Lmfs ---

= (10)

I IEDC

EDC RF I K I

2

= ∆

CCM operation : KRF < 1

I IEDC

EDC RF I K I

2

= ∆

DCM operation : KRF =1 peak

Ids peak

Ids

NPmin LmIover BsatAe

---×106 (turns)

= (11)

Aw Aw Aw Aw

Ae Ae

Ae Ae

(6)

Figure 8. Typical B-H characteristics of ferrite core (TDK/PC40)

Table 2. Typical cores for battery charger (For universal input range, 5V output and fs=100kHz)

(7) STEP-7 : Determine the number of turns for each output

Figure 9 shows the simplified diagram of the transformer.

First, determine the turns ratio (n) between the primary side and the secondary side.

where Np and Ns are the number of turns for primary side and reference output, respectively, Vo is the output voltage, VF is the diode (DR) forward voltage drop and Vsense is the maximum voltage drop in the output current sensing resistor.

Then, determine the proper integer for Ns so that the resulting Np is larger than Npmin obtained from equation (11).

The number of turns for Vcc winding is determined as

where Vcc* is the nominal value of the supply voltage of the FPS device, and VFa is the forward voltage drop of Da as defined in Figure 9. Since Vcc increases as the output load increases, it is proper to set Vcc* as Vcc start voltage (refer to the data sheet) to avoid triggering the over voltage protection during normal operation.

Figure 9. Simplified diagram of the transformer

With the determined turns of the primary side, the gap length of the core is obtained as

where AL is the AL-value with no gap in nH/turns2, Ae is the cross sectional area of the core as shown in Figure 8, Lm is specified in equation (6) and Np is the number of turns for the primary side of the transformer

(8) STEP-8 : Determine the wire diameter for each winding based on the rms current of each output.

The rms current of the n-th secondary winding is obtained as

where VRO and Idsrms are specified in step-3 and equations (8), Vo is the output voltage, VF is the diode (DR)) forward voltage drop and Dmax is specified in equation (5).

The current density is typically 5A/mm2 when the wire is Core Cross sectional

area

Window area Output power range EE13-Z 17.1 mm2 33.4 mm2 3-5W EI16-Z 19.8 mm2 38.8 mm2 3-5W EE16-Z 21.7 mm2 51.3 mm2 5-10W EI19-Z 24.0 mm2 54.4 mm2 5-10W

100 500

400

300

200

800 1600

0 0

M agnetic field H (A /m )

Flux density B (mT)

M agnetization C urves (typical) M aterial :PC 40

100 ℃ 120 ℃ 60 ℃ 25 ℃

n NP

Ns

--- VR0

Vo+VF+Vsense ---

= = (12)

Na Vcc*+VFa Vo+VF ---

=Ns1 (turns) ( )13

Np

NS -

VRO +

DR Na

Da +

VO - + VF - - VFa +

+ Vcc*

-

- Vsense +

) ( o F sense

s p

RO V V V

N

V = N + +

G 40πAe NP

2

1000Lm

--- 1 AL ---

 – 

 

 

= (mm) ( )14

Isrms Idsrms 1Dmax

Dmax

--- VRO Vo+VF

( )

---

= ( )15

(7)

long (>1m). When the wire is short with a small number of turns, a current density of 6-10 A/mm2 is also acceptable.

Avoid using wire with a diameter larger than 1 mm to avoid severe eddy current losses as well as to make winding easier.

For high current output, it is better to use parallel windings with multiple strands of thinner wire to minimize skin effect.

Check if the winding window area of the core, Aw (refer to Figure 8) is enough to accommodate the wires. Because bobbin, insulation tape and gaps between wires, the wire can not fill the entire winding window area. Typically the fill factor is about 0.15-0.2 for a battery charger. When additional dummy windings are employed for EMI shielding, the fill factor is reduced. The required winding window area (Awr) is given by

where Ac is the actual conductor area and KF is the fill factor.

If the required window (Awr) is larger than the actual window area (Aw), go back to the step-6 and change the core to a bigger one. Sometimes it is impossible to change the core due to cost or size constraints. If so, go back to step-4 and reduce Lm by increasing the ripple factor (KRF) or reducing the maximum duty ratio. Then, the minimum number of turns for the primary (Npmin) of the equation (11) will decrease, which results in the reduced required winding window area (Awr).

(9) STEP-9 : Choose the rectifier diode in the secondary side based on the voltage and current ratings.

The maximum reverse voltage and the rms current of the output rectifier diode (DR) are obtained as

where VDCmax, Dmax and Idsrms are specified in equations (3), (5) and (8), respectively, Vo is the output voltage, VF is the diode (DR) forward voltage and Vsense is the maximum voltage drop in the output current sensing resistor.

The typical voltage and current margins for the rectifier diode are as follows

where VRRM is the maximum reverse voltage and IF is the average forward current of the diode.

A quick selection guide for Fairchild Semiconductor rectifier diodes is given in table 3.

Table 3. Fairchild Diode quick selection table

(10) STEP-10 : Determine the output capacitor considering the voltage and current ripple.

The ripple current of the output capacitor (Co) is obtained as

where Io is the load current and IDrms is specified in equation (18). The ripple current should be smaller than the ripple current specification of the capacitor. The voltage ripple on the n-th output is given by

where Co is the output capacitance, Rc is the effective series resistance (ESR) of the output capacitor, Dmax and Idspeak are specified in equations (5) and (7), respectively, Io and Vo are the load current and output voltage, respectively, VF is the diode (DR) forward voltage and Vsense is the maximum voltage drop in the output current sensing resistor.

Sometimes it is impossible to meet the ripple specification with a single output capacitor due to the high ESR of the electrolytic capacitor. Then, additional LC filter stages (post filter) can be used. When using the post filters, be careful not to place the corner frequency too low. Too low a corner frequency may make the system unstable or limit the control bandwidth. It is typical to set the corner frequency of the post filter at around 1/10~1/5 of the switching frequency.

(11) STEP-11 : Design the RCD snubber.

When the power MOSFET is turned off, there is a high voltage spike on the drain due to the transformer leakage inductance. This excessive voltage on the MOSFET may lead to an avalanche breakdown and eventually failure of the FPS. Therefore, it is necessary to use an additional network to clamp the voltage.

The RCD snubber circuit and MOSFET drain voltage waveform are shown in Figure 10 and 11, respectively. The RCD snubber network absorbs the current in the leakage inductance by turning on the snubber diode (Dsn) once the MOSFET drain voltage exceeds the voltage of node X as depicted in Figure 10. In the analysis of snubber network, it is assumed that the snubber capacitor is large enough that its voltage does not change significantly during one switching Awr = Ac⁄KF (16)

VD Vo VDCmax⋅(Vo+VF+Vsense) VRO

--- +

= ( )17

IDrms Idsrms VDCmin

VRO

--- VRO Vo+VF+Vsense

( )

---

= ( )18

VRRM>1.3 VD (19) IF>1.5 IDrms (20)

Schottky Barrier Diode

Products VRRM IF Package

SB340 40 V 3 A TO-210AD

SB350 50 V 3 A TO-210AD

SB360 60 V 3 A TO-210AD

Icaprms = (IDrms)2Io2 (21)

Vo IoDmax Cofs

--- IdspeakVRORC Vo+VF+Vsense

( )

--- (22) +

=

(8)

cycle. The snubber capacitor used should be ceramic or a material that offers low ESR. Electrolytic or tantalum capacitors are unacceptable due to these reasons.

Figure 10. Circuit diagram of the snubber network

The first step in designing the snubber circuit is to determine the snubber capacitor voltage at the minimum input voltage and full load condition (Vsn). Once Vsn is determined, the power dissipated in the snubber network at the minimum input voltage and full load condition is obtained as

where Idspeak is specified in equation (8), fs is the FPS switching frequency, Llk is the leakage inductance, Vsn is the snubber capacitor voltage at the minimum input voltage and full load condition, VRO is the reflected output voltage and Rsn is the snubber resistor. Vsn should be larger than VRO and it is typical to set Vsn to be 2~2.5 times VRO. Too small a Vsn results in a severe loss in the snubber network as shown in equation (23). The leakage inductance is measured at the switching frequency on the primary winding with all other windings shorted.

Then, the snubber resistor with proper rated wattage should be chosen based on the power loss. The maximum ripple of the snubber capacitor voltage is obtained as

where fs is the FPS switching frequency. In general, 5~10%

ripple of the selected capacitor voltage is reasonable.

The snubber capacitor voltage (Vsn) of equation (26) is for the minimum input voltage and full load condition. When the converter is designed to operate in CCM under this condition, the peak drain current together with the snubber capacitor voltage decrease as the input voltage increases as shown in Figure 11. The peak drain current at the maximum

input voltage and full load condition (Ids2peak) is obtained as

where Pin, and Lm are specified in equations (1) and (6), respectively and fs is the FPS switching frequency.

The snubber capacitor voltage under maximum input voltage and full load condition is obtained as

where fs is the FPS switching frequency, Llk is the primary side leakage inductance, VRO is the reflected output voltage and Rsn is the snubber resistor.

Figure 11. MOSFET drain voltage and snubber capacitor voltage

From equation (26), the maximum voltage stress on the internal MOSFET is given by

where VDCmax is specified in equation (3).

Check if Vdsmax is below 85% of the rated voltage of the MOSFET (BVdss) as shown in Figure 12. The voltage rating of the snubber diode should be higher than BVdss. Usually, an ultra fast diode with 1A current rating is used for the snubber network.

Rsn Csn Np - Vsn

+ VDC

+ -

Dsn

Drain

GND FPS CDC

- VRO

+

+ Vds

- Llk VX

X

Psn (Vsn)2 Rsn --- 1

2---fsLlK(Idspeak)2 Vsn VsnVRO ---

= = (23)

Vsn Vsn CsnRsnfs ---

= (24)

Ids2peak 2 Pin fsLm ---

= (25)

Vsn2 VRO+ (VRO)2+2RsnLlkfs(Ids2peak)2 ---2

= (26)

VDC min

VRO Vsn

VDC max

VRO Vsn2

Idspeak

Ids2peak

Minimum input voltage

& Full load

Maximum input voltage

& Full load Ids2peak < Idspeak ==> Vsn2 < Vsn

Vdsmax = VDCmax+Vsn2 (27)

(9)

In the snubber design in this section, neither the lossy discharge of the inductor nor stray capacitance is considered.

In the actual converter, the loss in the snubber network is less than the designed value due to this effects.

Figure 12. MOSFET drain voltage and snubber capacitor voltage

(12) STEP-12 : Design the Control circuit.

In general, a battery charger employs constant current (CC) / constant voltage (CV) control circuit for an optimal charge of a battery. This design note presents two basic CC/CV control circuits for FPS flyback converters. A simple, low cost circuit using a transistor and shunt regulator (KA431) is presented first. The second circuit features highly accurate current control using an op amp together with a shunt regulator (KA431) and secondary bias winding. In the circuit analysis, it is assumed that the CTR of the opto-coupler is 100%.

(a) Transistor and regulator (KA431) scheme

Figure 13 shows the CC/CV control circuit using a transistor and KA431 for 5.2V/0.65A output application. This circuit is widely used when low cost and simplicity are major concerns. Since the transistor base-emitter voltage drop depends on the temperature, a temperature compensation circuit is required for temperature stability. To turn on the transistor (Q), about 0.7V voltage drop across the sensing resistor (Rsense) is required and this current control circuit should be used for output currents below 1A due to the power dissipated in current sense resistor. For output currents greater than 1A, or if output current accuracy and

temperature stability are a key factor, the op amp current control circuits shown in Figure 15 should be used.

Figure 13. Transistor and KA431 CC/CV control

Constant voltage (CV) control : The voltage divider network of R1 and R2 should be designed to provide 2.5V to the reference pin of the KA431. The relationship between R1 and R2 is given by

where Vo is the output voltage.

By choosing R1 to be 2.2kΩ, R2 is obtained as

The feedback capacitor (CF) introduces an integrator for CV control. To guarantee stable operation, CF of 470nF is chosen.

The resistors Rbias and Rd should be designed to provide proper operating current for the KA431 and to guarantee the full swing of the feedback voltage for the FPS device chosen.

In general, the minimum cathode voltage and current for the KA431 are 2.5V and 1mA, respectively. Therefore, Rbias and Rd should be designed to satisfy the following conditions.

0 V

VDC max

VRO Vsn2

Effect of stray inductance (5-10V) BVdss

Voltage Margin > 10% of BVdss

NS DR

CO

KA431 817A

Rd

Rbias

R1

R2 CF

VO LP

CP

Rsense

Rbase Q

RTH

CB vFB

1:1 FPS

RB

GND IFB

Io

250uA 56ΩΩΩΩ 510ΩΩΩΩ

470nF KSP2222

10kΩΩΩΩ

510ΩΩΩΩ ΩΩΩ

5.2V / 0.65A

2.2kΩΩΩΩ

2kΩΩΩΩ

R2 2.5 R1

Vo2.5 ---

= (28)

R2 2.5 2.2k⋅ Ω

5.2V2.5V

--- 2k

= =

VoVOP2.5 Rd

--->IFB (29) VOP

Rbias

--->1mA (30)

(10)

where Vo is the output voltage, VOP is opto-diode forward voltage drop, which is typically 1V and IFB is the feedback current of FPS. With IFB=0.25mA (FSD210), Rd and Rbias are determined as 56Ω and 510Ω, respectively.

Constant Current (CC) control : The current control circuit is shown in detail in Figure 14. The CC control is implemented using a transistor. Because the transistor base- emitter voltage drop varies with the temperature, negative thermal coefficient (NTC) thermistor is used for a temperature compensation.

Figure 14. Current control circuit in detail

When the voltage across the sensing resistor is sufficient to turn on the transistor, CC controller is enabled while CV controller is disabled. Then, the KA431 consumes very small current and most of the currents through Rd and Rbias flow into the collector of the transistor Q. By assuming that the feedback voltage of FPS (VFB) is in the middle of its operating range, half of the FPS feedback current (IFB) sinks into the opto-coupler transistor. Since it is also assumed that the CTR of the opto-coupler is 100%, the transistor collector current is given by

where IFB is the feedback current of FPS, VOP is opto-diode forward voltage drop, which is typically 1V.

From the circuit in Figure 14, IC is obtained as

By assuming that the current gain (β) of Q is 100, the transistor base current is obtained as

The voltage drop in the sensing resistor (Vsense) should be set to be 40-100mV higher than the transistor base-emitter voltage (VBE) at room temperature (25°C). The actual transistor base-emitter voltage (VBE) temperature is measured at room temperature as 0.608V with IC of 2.1mA and Vsense is determined to be 0.650V.

With the Vsense chosen, the sensing resistor (Rsense) is obtained as

where Io is SMPS output current.

It is typical to design the NTC thermistor so that the current through the thermistor would be about 3-6 times of the transistor base current at room temperature. The resistance of the thermistor at room temperature (RTH) is determined as 10 kΩ. The current through the thermistor is obtained as

The base resistor is determined by

Variations in the junction temperature of Q will cause variations in the value of controlled output current (Io). The base-emitter voltage decreases with increasing temperature at a rate of approximately 2mV/°C. When the base-emitter voltage is changed to VBET as the temperature changes to T

°C, the thermistor resistance at T °C required to compensate this variation is given by

With -2mV/°C, VBE reduces to 0.508V from 0.608V as temperature increases from 25°C to 75°C. From equation KA431

Rd Rbias

Rsense

Rbase Q

RTH

Io = 0.65A

510ΩΩΩΩ 56ΩΩΩΩ

KSP2222 10kΩΩΩΩ

510ΩΩΩΩ 1ΩΩΩΩ

IRTH

b e

c IFB /2

+ VOP

- IC

IB VBE

Vsense

IC (IFBRd)⁄2+Vop Rbias

--- 1 2--- IFB +

= (31)

IC (250µA 56⋅ Ω)⁄2+1V

510

--- 1

2--- 250⋅ µA

+ 2.1mA

= =

IB IC

---β 2.1mA

---100 21uA

= = = (32)

Rsense Vsense Io

--- 0.65V 0.65A --- 1

= = = (33)

IRTH VBE

RTH

--- 0.608V

10k

--- 61µA

= = = (34)

Rbase VsenseVBE VBE RTH ---+IB

--- 0.65V0.608V 0.608V

10k

---+21µA

--- 513

= = = (35)

RTHT VBET

VsenseVBET Rbase ---IB ---

= (36)

(11)

(36), the resistance of the thermistor at 75°C to keep the same output current is given by

NTC thermistor 103Χ2 from DSC is chosen for the compen- sation, whose resistance is 10kΩ at 25°C and 1.92kΩ at 75°C.

(b) OP amp and shunt regulator (KA431) scheme

Figure 15 shows a 4.2 V, 0.8A CC/CV control circuit using the LM358 dual op amp shunt regulator (KA431). This circuit provides higher accuracy compared with the simple transistor circuit. Power loss is lower and efficiency is better because smaller resistance values can be used for sense resistor Rsense. The shunt regulator (KA431) is used as a voltage reference for an accurate control.

Constant voltage (CV) control : The Output voltage is sensed by R1 and R2 and then compared by OP amp LM358B to reference of 2.5V. The output of the OP amp drives current through D2 and Rd into the LED of the opto- coupler. The voltage divider network of R1 and R2 should be designed to provide 2.5V to the reference pin of the KA431.

The relationship between R1 and R2 is given by

where Vo is the output voltage.

By choosing R1 to be 680Ω, R2 is obtained as

CF2, RF2, and R6 compensate the voltage control loop.

Constant Current (CC) control : The voltage drop across the sensing resistor (Rsense) is given by

It is typical to set Vsense as 0.1-0.2V.

Since the inverting input of OP amp is virtually grounded, the relationship between R4 and R5 is given by

By choosing R5 as 33kΩ, R4 is obtained as 2.1kΩ. CF2, RF2, and R6 compensate the current control loop.

0.508V

0.65V0.508V

---513 21µA

---=1.99k

R2 2.5 R1

Vo2.5 ---

= (37)

R2 2.5⋅680

4.2V–2.5V --- 1k

= =

Vsense = IoRsense ( )38

R4 VsenseR5 ---2.5

= (39)

(12)

Figure 15. CC/CV control using OP amp and shunt regulator

NS DR

CO

H 11A 81 7A Rd

R1

R2 VO LP

CP Rsen se Db ias

Cbia s Vb ias

R3

K A 431 VR E F= 2 .5 V R4

R5 CF 1

CF 2 L M 3 58 A

L M 3 58 B 1

3 2

4 8

5 6 7

IO Nb ias

CB vF B

1 :1

F P S

RB

G N D IF B

1N 4 148

RF 1

0 .2 ΩΩΩΩ

4.2V

0.8 A

6 8 0ΩΩΩΩ

1 .0kΩΩΩΩ 4 .7 kΩΩΩΩ

RF 2 4 .7 kΩΩΩΩ

0.1 uF

1 kΩΩΩΩ

R6 1 0 0 kΩΩΩΩ

20 0ΩΩΩΩ

0 .1 u F

3 3kΩΩΩΩ 2 .1 kΩΩΩΩ

1N 4 14 8 D1

D2

(13)

- Summary of symbols -

Aw : Winding window area of the core in mm2 Ae : Cross sectional area of the core in mm2 Bsat : Saturation flux density in tesla.

Co : Output capacitor

Dmax : Maximum duty cycle ratio Eff : Estimated efficiency fL : Line frequency

fs : Switching frequency of FPS

Idspeak : Maximum value of peak current through MOSFET at the minimum input voltage condition Ids2peak : Maximum value of peak current through MOSFET at the maximum input voltage condition Idsrms : RMS current of MOSFET

Ids2 : Maximum peak drain current at the maximum input voltage condition.

Iover : FPS current limit level.

Iserms : RMS current of the secondary winding

IDrms : Maximum rms current of the output rectifier diode Icaprms : RMS Ripple current of the output capacitor Io : Output load current

KRF : Current ripple factor

Lm : Transformer primary side inductance Llk : Transformer primary side leakage inductance

Losssn : Maximum power loss of the snubber network in normal operation

Npmin : The minimum number of turns for the transformer primary side to avoid saturation Np : Number of turns for primary side winding

Ns : Number of turns for the output winding Na : Number of turns for the Vcc winding Po : Maximum output power

Pin : Maximum input power

Rc : Effective series resistance (ESR) of the output capacitor.

Rsn : Snubber resistor

RL : Effective total output load resistor of the controlled output Vlinemin : Minimum line voltage

Vlinemax : Maximum line voltage VDCmin : Minimum DC link voltage VDCmax : Maximum DC line voltage

Vdsnom : Maximum nominal MOSFET voltage Vo : Output voltage

VF : Forward voltage drop of the output rectifier diode.

Vcc* : Nominal voltage for Vcc

VFa : Diode forward voltage drop of Vcc winding VD : Maximum voltage of the output rectifier diode VRO : Output voltage reflected to the primary

Vsn : Snubber capacitor voltage under minimum input voltage and full load condition Vsn2 : Snubber capacitor voltage under maximum input voltage and full load condition Vdsmax : Maximum voltage stress of the MOSFET

参照

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The output voltage is indirectly sensed by sampling the transformer winding voltage (V SH ) around the end of diode current discharge time, as illustrated in Figure 4..

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ON Semiconductor makes no warranty, representation or guarantee regarding the suitability of its products for any particular purpose, nor does ON Semiconductor assume any liability

ON Semiconductor makes no warranty, representation or guarantee regarding the suitability of its products for any particular purpose, nor does ON Semiconductor assume any liability

Should Buyer purchase or use ON Semiconductor products for any such unintended or unauthorized application, Buyer shall indemnify and hold ON Semiconductor and its officers,

ON Semiconductor makes no warranty, representation or guarantee regarding the suitability of its products for any particular purpose, nor does ON Semiconductor assume any liability